Physical Properties of Crystals: Their Representation by Tensors and Matrices |
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Page 64
... force on each small volume dv of the crystal are therefore , from ( 26 ) , = dF1 dv.μo 21 H1 ( H2 / x1 ) , Putting dv = dF2 dv.po11 H1 ( ƏH1 / dx2 ) , = dFs = 0 . a dx2 , where a is the cross - sectional area of the rod , we find for ...
... force on each small volume dv of the crystal are therefore , from ( 26 ) , = dF1 dv.μo 21 H1 ( H2 / x1 ) , Putting dv = dF2 dv.po11 H1 ( ƏH1 / dx2 ) , = dFs = 0 . a dx2 , where a is the cross - sectional area of the rod , we find for ...
Page 65
... force applies to every small element of the crystal , and that therefore , owing to the finite size of the crystal , the forces on different parts of the crystal will , in general , be different both in magni- tude and direction . They ...
... force applies to every small element of the crystal , and that therefore , owing to the finite size of the crystal , the forces on different parts of the crystal will , in general , be different both in magni- tude and direction . They ...
Page 83
... force will be transmitted across each face of the cube , exerted by the material outside the cube upon the material inside the cube . The force transmitted across each face may be resolved into three components . Consider first the ...
... force will be transmitted across each face of the cube , exerted by the material outside the cube upon the material inside the cube . The force transmitted across each face may be resolved into three components . Consider first the ...
Contents
THE GROUNDWORK OF CRYSTAL PHYSICS | 3 |
EQUILIBRIUM PROPERTIES | 51 |
ELECTRIC POLARIZATION | 68 |
18 other sections not shown
Common terms and phrases
angle anisotropic applied axial vector centre of symmetry Chapter coefficients conductivity constant crystal classes crystal properties crystal symmetry cube cubic crystals defined denoted diad axis dielectric dijk direction cosines dummy suffix elastic electric field ellipsoid equation example force given grad H₁ H₂ heat flow Hence hexagonal homogeneous indicatrix isothermal isotropic k₁ magnetic magnitude matrix notation measured moduli monoclinic number of independent Onsager's Principle optical activity orientation orthorhombic Ox₁ P₁ parallel Peltier permittivity perpendicular photoelastic effect piezoelectric effect plane plate polarization principal axes produced pyroelectric pyroelectric effect quantities radius vector referred refractive index relation representation quadric represented right-handed rotation S₁ scalar second-rank tensor set of axes shear strain stress suffix notation surface susceptibility symmetry elements Table temperature gradient thermal expansion thermodynamics thermoelectric effects Thomson heat tion transformation law triclinic trigonal uniaxial values x₁ Young's Modulus zero